Independent control of both index and dispersion in gradient index optics

ABSTRACT

Three or more base optical materials are selectively combined into a trans-gradient index (GRIN) optical element (e.g., a lens). A wavelength-dependent index of refraction for light propagating perpendicular to the three or more optical materials equals: a volume fraction of a first optical material multiplied by a refractive index of the first optical material, plus a volume fraction of a second optical material multiplied by a refractive index of the second optical material, plus one minus the volume fraction of the first optical material and the volume of the second optical material all multiplied by the refractive index of a third optical material. The wavelength-dependent index of refraction distribution and a refractive index dispersion through the GRIN optical element may be independently specified from one another. A local refractive index at any point in the optical element is a fixed function of a refractive index of each individual optical material.

CROSS REFERENCE TO RELATED APPLICATION

This application claims the benefit of U.S. Provisional PatentApplication No. 62/408,099 filed on Oct. 14, 2016. The ProvisionalApplication and all references cited herein are hereby incorporated byreference into the present disclosure.

GOVERNMENT INTEREST

The embodiments herein may be manufactured, used, and/or licensed by orfor the United States Government without the payment of royaltiesthereon.

BACKGROUND Technical Field

The embodiments herein generally relate to optics, and more particularlyto gradient index optics.

Description of the Related Art

Engineering a gradient index (GRIN) distribution in a lens is a knownpotential benefit to optical design. In a GRIN lens, the material is nota constant throughout the lens, whereby light rays bend within the lensas well as at the surface. Primary, seminal works on GRIN opticsconcentrated on descriptions of the refractive index distribution withina lens as a mathematical construct as has been described by Sands, P.J., “Inhomogeneous lenses II. Chromatic paraxial aberrations,” J. Opt.Soc. Am. 61 (6) 777-783 (1971). The research is based on an extension ofthird-order aberration theory in optics, which treats the behavior oflight rays as a combination of perfect behavior plus aberrations, wheredifferent aberrations are defined according to algebraic expressionswhich have different contributions from each lens element in an opticalsystem. An algebraic description of these light rays required asimilarly algebraic description of the index function and its variationwith color. To be compatible with the treatment, the index function andits variation with color was simply assigned a multi-order polynomialexpansion function, as further described by Krishna, K. S. R. et al.,“Chromatic aberrations of radial gradient-index lenses. 1. Theory,”Appl. Opt. 35 (7) 1032-6 (1996). A GRIN lens may be approximated thisway, after the fact. However, what is missing is how to predict whatthose properties would be for a lens, because in such a treatment thereis no connection to the materials which make up the GRIN.

SUMMARY

In view of the foregoing, an embodiment herein provides a methodcomprising providing three or more base optical materials comprising afirst base optical material, a second base optical material, and a thirdbase optical material; selectively combining the three or more baseoptical materials into a set of trans-GRIN materials; and using the setof trans-GRIN materials to independently control both an index ofrefraction distribution and an optical dispersion distribution through aGRIN optical element. A wavelength-dependent index of refraction forlight propagating perpendicular to the three or more base opticalmaterials may equal: a volume fraction of the first base opticalmaterial multiplied by a refractive index of the first base opticalmaterial, plus a volume fraction of the second base optical materialmultiplied by a refractive index of the second base optical material,plus one minus the volume fraction of the first base optical materialand the volume of the second base optical material all multiplied by therefractive index of the third base optical material.

A local refractive index at any point in the GRIN optical element is afixed function of a refractive index of each individual base opticalmaterial of the three or more base optical materials. The three or morebase optical materials may comprise polymer materials. The three or morebase optical materials may comprise any of polyethylene naphthalate, anisomer thereof, a polyalkylene terephthalate, a polyimide, apolyetherimide, a styrenic polymer, a polycarbonate, apoly(meth)acrylate, a cellulose derivative, a polyalkylene polymer, afluorinated polymer, a chlorinated polymer, a polysulfone, apolyethersulfone, polyacrylonitrile, a polyamide, polyvinyl acetate, apolyether-amide, a styrene-acrylonitrile copolymer, a styrene-ethylenecopolymer, poly(ethylene-1,4-cyclohexylenedimethylene terephthalate), anacrylic rubber, isoprene, isobutylene-isoprene, butadiene rubber,butadiene-styrene-vinyl pyridine, butyl rubber, polyethylene,chloroprene, epichlorohydrin rubber, ethylene-propylene,ethylene-propylene-diene, nitrile-butadiene, polyisoprene, siliconrubber, styrene-butadiene, and urethane rubber. The three or more baseoptical materials may comprise glass. The three or more base opticalmaterials may comprise different materials.

Another embodiment provides a trans-GRIN lens comprising a selectivecombination of three or more base optical materials comprising a firstbase optical material, a second base optical material, and a third baseoptical material, wherein a wavelength-dependent index of refraction forlight propagating perpendicular to the combined three or more baseoptical materials comprises a combination of: a volume fraction of thefirst base optical material combined with a refractive index of thefirst base optical material, a volume fraction of the second baseoptical material combined with a refractive index of the second baseoptical material, and one minus the combined volume fraction of thefirst base optical material and the volume of the second base opticalmaterial all multiplied by the refractive index of the third baseoptical material. The wavelength-dependent index of refractiondistribution and a refractive index dispersion through the GRIN lens areindependently specified from one another. A local refractive index atany point in the lens is a fixed function of a refractive index of eachindividual base optical material of the three or more base opticalmaterials. The three or more base optical materials may comprise polymermaterials. The polymer materials may comprise thermoplastic polymericmaterials. The three or more base optical materials may comprise glass.The three or more base optical materials may comprise differentmaterials.

Another embodiment provides a system comprising a fusing device thatselectively combines at least three base optical materials into one GRINlens, and a control unit that drives the fusing device to independentlycontrol both an index of refraction distribution and an opticaldispersion distribution through the GRIN lens. The at least three baseoptical materials comprise a first base optical material, a second baseoptical material, and a third base optical material, wherein the indexof refraction distribution (n(λ)²) for light propagating perpendicularto the combined at least three base optical materials is represented by:n(λ)₂=(φ_(A)n_(A)(λ)²+φ_(B)n_(B)(λ)²+(1−φ_(A)−φ_(B))n_(C)(λ)², andwherein φ_(A) is a volume fraction of the first base optical material,φ_(B) is a volume fraction of the second base optical material, φ_(C) isa volume fraction of the third base optical material, n_(A)(λ)² is arefractive index of the first base optical material, n_(B)(λ)² is arefractive index of the second base optical material, and n_(C)(λ)² is arefractive index of the third base optical material. In an embodiment,nA(λ)<nB(λ)<nC(λ), and volume fractions φA and φB may be bothnon-negative values whose sum is less than 1. The at least three baseoptical materials may comprise polymer materials. The at least threebase optical materials may comprise glass.

These and other aspects of the embodiments herein will be betterappreciated and understood when considered in conjunction with thefollowing description and the accompanying drawings. It should beunderstood, however, that the following descriptions, while indicatingpreferred embodiments and numerous specific details thereof, are givenby way of illustration and not of limitation. Many changes andmodifications may be made within the scope of the embodiments hereinwithout departing from the spirit thereof, and the embodiments hereininclude all such modifications.

BRIEF DESCRIPTION OF THE DRAWINGS

The embodiments herein will be better understood from the followingdetailed description with reference to the drawings, in which:

FIG. 1 is a block diagram of a system, according to an embodimentherein;

FIG. 2 is a flow diagram illustrating a method, according to anembodiment herein;

FIG. 3A is a graph illustrating a first index vs. dispersion curve,according to an embodiment herein;

FIG. 3B is a graph illustrating a second index vs. dispersion curve,according to an embodiment herein;

FIG. 3C is a graph illustrating a third index vs. dispersion curve,according to an embodiment herein;

FIG. 4A is a graph illustrating a fourth index vs. dispersion curve,according to an embodiment herein;

FIG. 4B is a graph illustrating an index slope vs. index curve,according to an embodiment herein;

FIG. 5A is a cross-sectional diagram illustrating stacked opticalmaterials, according to an embodiment herein;

FIG. 5B is a cross-sectional diagram illustrating a ternary material,according to an embodiment herein; and

FIG. 5C is a cross-sectional diagram illustrating a material with twodopants, according to an embodiment herein.

DETAILED DESCRIPTION

The embodiments herein and the various features and advantageous detailsthereof are explained more fully with reference to the non-limitingembodiments that are illustrated in the accompanying drawings anddetailed in the following description. Descriptions of well-knowncomponents and processing techniques are omitted so as to notunnecessarily obscure the embodiments herein. The examples used hereinare intended merely to facilitate an understanding of ways in which theembodiments herein may be practiced and to further enable those of skillin the art to practice the embodiments herein. Accordingly, the examplesshould not be construed as limiting the scope of the embodiments herein.

An embodiment herein provides an optical lens configuration technique,enabling an optical engineer to tailor both the refractive indexdistribution and refractive index dispersion within an optical element,independently. The embodiments herein provide a trans-GRIN lens, whichuses three or more base materials, and blends them in a way that allowsfor independent control of both the index and dispersion throughout thelens. The canonical literature for GRIN lens design generally fails toconnect GRIN distributions with material distributions, which theembodiments herein overcome. Referring now to the drawings, and moreparticularly to FIGS. 1 through 5C, where similar reference charactersdenote corresponding features consistently throughout the figures, thereare shown exemplary embodiments.

The use of three or more base optical materials within a single opticalelement to control both an index distribution and, independently, theoptical dispersion distribution throughout the element volume, asprovided by the embodiments herein, is a departure from conventionalGRIN technology. Optical dispersion is the variation of the refractiveindex with wavelength. All materials exhibit dispersion, which meanseach lens element in a GRIN lens treats different wavelengths of lightdifferently. Any system, GRIN or otherwise, designed for more than onewavelength must account for this effect.

A GRIN lens comprising two materials may be designed to control therelative concentration of the two component materials, at a length scalemuch smaller than the wavelength of light. An example two componentpolymer GRIN lens and method of fabrication is described in U.S. Pat.No. 7,002,754, the complete disclosure of which, in its entirety, isherein incorporated by reference. In such cases the local refractiveindex at any point is some fixed function of the refractive index ofeach individual material. For example, in a nanolayered system ofpolymers A and B, where each layer is much thinner than the wavelengthof light, the wavelength-dependent index of refraction n(λ) for lightpropagating perpendicular to the layers is given by:n(λ)²=φ_(A) n _(A)(λ)²+(1−φ_(A))n _(B)(λ)²  (1)where φA is the volume fraction of polymer A, nA(λ) is the refractiveindex of polymer A, and nB(λ) is the refractive index of polymer B.Since φA is a volume fraction, its value is between 0 and 1. Moreover, aGRIN can be created by generating a position-dependent variation in therelative weight fraction φA(r) of polymer A. Once defined, however, thedispersion distribution dn(r)/dλ of such a GRIN is fixed, because theindex depends on the single position-dependent variable φA(r). In otherwords, since the index for a GRIN blended from A and B depends on thesingle variable φA then this variable also describes all the dispersioninformation, as well.

With a given material pair to generate the GRIN effect, however, thereis a fixed relationship between the index distribution and thedistribution of dispersion. The bandwidth over which achromaticperformance can be achieved is limited to the fixed relationship betweenthe material pair and their dispersion curves.

The model given in Eq. (1) is only one of many models that can relatethe volume fraction φA to index. Also, there are other common GRINsystems, such as ion-diffused glass systems, whose index can't bedescribed as a simple, linear combination of two dispersion curves.However, what most of these systems share is the single-parameterdependence of index on position, such as the relative concentration ofthe mobile ion in ion-diffused glasses. With only a single parameter todescribe the index, the fixed relationship between index and dispersionremains.

In the trans-GRIN methodology provided by the embodiments herein, Eq.(1) is expanded to include the addition of a third constituent material.The index for a ternary material system can be described by:n(λ)²=φ_(A) n _(A)(λ)²+φ_(B) n _(B)(λ)²+(1−φ_(A)−φ_(B))n _(C)(λ)²  (2)where it will be assumed that nA(λ)<nB(λ)<nC(λ), and the volumefractions φA and φB make physical sense; i.e., that they are bothnon-negative values whose sum is less than 1, with the constraint thatφC is given by (1−φA−φB).

A consequence of this model is that there are identical values of indexachieved by a whole set of different materials. Since nB(λ) lies betweenthe values for A and C, for example, one can achieve nB(λ) byconstructing a pure B material (φB=1, φA=φC=0) or by having no Bmaterial, and blending A and C in just the right amounts to average outto nB(λ). Depending on the nature of the three pure materials, these twodifferent choices could have vastly different dispersion values.

The freedom afforded by the third material is that, for a range of indexvalues between the minimum nA and maximum nC values of index, the indexn and dispersion dn/dλ may be selected independently. For example, amaterial with the same intermediate index nX can be achieved with eithera relatively A-rich or a relatively C-rich mixture. When the A materialhas less dispersion than the C material, the former mixture will haveless dispersion than the latter, affording optical engineers a choice ofdispersion values for the same index value nX. An immediate extension ofthis concept is that, should a fourth material be added, the index, thefirst-order dispersion, and the second-order dispersion d²n/dλ² may bespecified independently. For each new material added to a blend, anadditional order of the dispersion may be controlled. The above processdescribes the origin of material combinations which may, as a set, beused to fabricate a gradient index optical element. The processes offabricating a GRIN optic are separate, and may include: (a) stacking,molding, and shaping a multilayered polymer lens, (b) cutting andpolishing ion-exchanged glass blanks (rods, flats, or slumped flats)containing multi-component diffused species, (c) additive manufacturingtechniques, such as ink-jet printing, which might start with print headsthat contain (i) pre-mixed trans-GRIN materials, or (ii) base materials,to form trans-GRIN materials simultaneously during the printing of theGRIN element, or (d) any other process which leverages the combinationof three or more materials to provide independent control of both indexand dispersion distributions throughout a GRIN optic.

FIG. 1 is a block diagram of a system 10, according to an embodimentherein. The system 10 comprises a fusing device 15 that selectivelycombines at least three base optical materials 25 into one trans-GRINlens 30. The fusing device 15 receives each of the base opticalmaterials 25, which may be configured as composite films comprising raw(pure) materials A, B, and C. Each composite film comprises a differentrefractive index. An ordered set of these multilayered composite filmsare assembled into a hierarchical multilayered composite GRIN sheet 26with the desired index gradient. An example of a GRIN sheet 26 arrangedin a composite stack 70 is shown in FIG. 5A. These multilayeredcomposite GRIN sheets 26 are shaped into a lens 30. Sheet 26 maycomprise a whole set of different materials, each with its own ratio ofA_(x):B_(y):C_(z):<D:etc.>, which are combined into a GRIN lens 30. Eachmultilayered polymer composite film may comprise up to 500,000 layersalternating between at least three types of materials: A, B, and C.

A control unit 20 drives the fusing device 15 to independently controlboth an index of refraction distribution and an optical dispersiondistribution through the GRIN lens 30. The at least three base opticalmaterials 25 comprise a first base optical material A, a second baseoptical material B, and a third base optical material C, wherein theindex of refraction distribution (n(λ)²) for light propagatingperpendicular to the combined at least three base optical materials isrepresented by Eq. (2). Intervening components, devices, and sub-systemsmay be included in between the various components and devices shown inFIG. 1, but are not depicted for the sake of clarity.

FIG. 2, with reference to FIG. 1, is a flow diagram illustrating amethod 50 comprising providing (52) three or more base optical materials25 comprising a first base optical material A, a second base opticalmaterial B, and a third base optical material C. The method 50 mayfurther comprise selectively combining (54) the three or more baseoptical materials 25 into a set of trans-GRIN materials 26, wherein awavelength-dependent index of refraction for light propagatingperpendicular to the three or more base optical materials 25 isrepresented by Eq. (2).

The method 50 may further comprise using (56) the trans-GRIN materials26 to independently control both an index of refraction distribution andan optical dispersion distribution through a GRIN optical element (e.g.,GRIN lens 30). A local refractive index at any point in the GRIN opticalelement (e.g., GRIN lens 30) is a fixed function of a refractive indexof each individual base optical material of the three or more baseoptical materials 25. The three or more base optical materials 25 maycomprise glass, in one example. The three or more base optical materials25 may comprise different materials, in another example. The three ormore base optical materials 25 may include blends of two or morepolymers or copolymers, and may comprise components that aresubstantially miscible, thus not affecting the transparency of theblend. Example polymeric materials include a poly(vinylidene fluoride)(PVDF) and copolymers thereof, a poly(methyl methacrylate), apoly(ethylene naphthalate) (PEN), and a polycarbonate.

The three or more base optical materials 25 may comprise polymermaterials, in an example. As used herein, the term “polymer” may referto a material having a weight average molecular weight (Mw) of at least5,000. In another example, the polymer comprises an organic polymermaterial. In an embodiment, the polymer materials may comprisethermoplastic polymeric materials, such as glassy, crystalline, orelastomeric materials.

Furthermore, in another example, the three or more base opticalmaterials 25 may comprise any of polyethylene naphthalate, an isomerthereof, a polyalkylene terephthalate, a polyimide, a polyetherimide, astyrenic polymer, a polycarbonate, a poly(meth)acrylate, a cellulosederivative, a polyalkylene polymer, a fluorinated polymer, a chlorinatedpolymer, a polysulfone, a polyethersulfone, polyacrylonitrile, apolyamide, polyvinyl acetate, a polyether-amide, a styrene-acrylonitrilecopolymer, a styrene-ethylene copolymer,poly(ethylene-1,4-cyclohexylenedimethylene terephthalate), an acrylicrubber, isoprene, isobutylene-isoprene, butadiene rubber,butadiene-styrene-vinyl pyridine, butyl rubber, polyethylene,chloroprene, epichlorohydrin rubber, ethylene-propylene,ethylene-propylene-diene, nitrile-butadiene, polyisoprene, siliconrubber, styrene-butadiene, and urethane rubber.

FIGS. 3A through 3C, with reference to FIGS. 1 and 2, are graphsillustrating index vs. dispersion curves, according to the embodimentsherein. FIG. 3A shows bolded curves 60 a, 60 b which represent thedispersion functions of two base materials which may be combined to forma set of materials with index curves that lie between them. While theseparticular curves correspond to the optical polymers styreneacrylonitrile (SAN) and poly(methyl methacrylate) (PMMA), it isunderstood that the concept is generalized to any two materials whichmay be combined to form a gradient index optical element. Theintermediate, thinner curve 60 c in FIG. 3A represents one particularblend of SAN and PMMA, with ˜54% SAN. FIG. 3B contains the same threecurves 60 a, 60 b, 60 c as depicted in FIG. 3A with the addition of athird bold curve 60 d representing a third optical polymer, TOPAS®material. TOPAS® material has an index of refraction equal to that ofthe intermediate curve 60 c at a wavelength of approximately 0.5 μm.TOPAS® material, however, is less dispersive. In other words, the slopeof the TOPAS® material dispersion curve 60 d is shallower than the slopeof the 54% SAN:PMMA dispersion curve 60 c. FIG. 3C illustrates, as thinlines, the dispersion curves 60 e for a family of materials which wouldbe generated if one were to blend TOPAS and 54% SAN:PMMA together, inanalogy to the way in which SAN and PMMA are blended together in FIG.3A. All the intermediate materials have identical index values at thewavelength of approximately 0.5 μm, but each has a different dispersion.

FIGS. 4A and 4B, with reference to FIGS. 1 through 3C, represent thebroader range of materials offered by a ternary material combination,according to an embodiment herein. FIG. 4A depicts the dispersion curves61 a, 61 b, 61 c of materials A, B, and C (which for the sake ofillustrative values represent PMMA, SAN, and TOPAS® material in thesecurves, respectively). Also depicted by tangent lines 62 a, 62 b, 62 care the slopes of these curves 61 a, 61 b, 61 c, respectively, at aspecific, design wavelength of approximately 0.5 μm. In FIG. 4B, theshaded area 65 represents the combinations of index and dispersionavailable to a ternary blend of optical materials 25 provided by theembodiments herein. Each vertex (denoted by a triangle, circle, andsquare) of the shaded area 65 represents one of the three, basematerials, as given by the values of FIG. 4A. Each edge of the polygon(which, strictly speaking, would be slightly curved) represents thepossible binary combinations of the two base materials which theyconnect. For example, the longest edge between material A (triangle) andmaterial B (square) represents the all values accessed by a binarycombination of A and B. By adding the third material C, however, oneadds not just the two extra edges on this plot—it opens up the entirespace bounded between them. The greater the separation between theoriginal vertices, the greater the area afforded by a ternary mixtureamong them, and the greater choice of material values afforded to anoptical design engineer. The family of curves illustrated in FIG. 3C arerepresented on FIG. 4B as the vertical line which connects vertex C(TOPAS® material) to the AB edge. All the materials along this line havethe same index value at approximately 0.5 μm but different dispersionvalues, which demonstrates the ability to independently control bothindex and dispersion throughout a GRIN optical element, in accordancewith the embodiments herein.

FIGS. 5A through 5C, with reference to FIGS. 1 through 4B, illustrateseveral cross-sectional diagrams illustrating base optical materials A,B, and C arranged in different ways to form an A:B:C ternary blend 70according to an embodiment herein. In FIG. 5A, for example, materials A,B, and C are layered with a period small enough (<λ/10) that thecomposite blend 70 acts as an effective medium. The composite blend 70may be formed by extruding and layering materials A, B, and C. Themultilayered polymer composite films may be fabricated with a range ofrefractive indexes and an arbitrarily small index difference betweenthem. In one example, this may be accomplished by altering the relativethicknesses of the A, B, and C layers. Similarly, FIG. 5B shows anotherembodiment of a ternary material—subwavelength doping of materials B andC into a host A, in such a way that local volumes (<(λ/10)³) havecontrolled volume fractions of B and C. FIG. 5C represents a materialwith two dopants which could be co-diffused into a host to control itsoptical properties. In each of FIGS. 5A through 5C, the diagramsrepresent a single ternary combination. A trans-GRIN lens would befabricated through the assembly of a whole set of these combinations,utilizing the independent control of index and dispersion to meetoptical design goals.

The embodiments herein combine three or more base materials 25 into asingle trans-GRIN lens 30. While a two-material GRIN blend may provideflexibility in designing a customizable refractive index profile insidea lens, a three-material (or higher) GRIN lens 30, as provided by theembodiments herein, provides the degrees of freedom necessary toindependently specify the dispersion profile inside the lens 30.

The foregoing description of the specific embodiments will so fullyreveal the general nature of the embodiments herein that others may, byapplying current knowledge, readily modify and/or adapt for variousapplications such specific embodiments without departing from thegeneric concept, and, therefore, such adaptations and modificationsshould and are intended to be comprehended within the meaning and rangeof equivalents of the disclosed embodiments. It is to be understood thatthe phraseology or terminology employed herein is for the purpose ofdescription and not of limitation. Therefore, while the embodimentsherein have been described in terms of preferred embodiments, thoseskilled in the art will recognize that the embodiments herein may bepracticed with modification within the spirit and scope of the appendedclaims.

What is claimed is:
 1. A method comprising: providing a plurality ofbase optical materials including a first base optical material, a secondbase optical material, and a third base optical material; combining theplurality of base optical materials into a set of trans-gradient index(GRIN) materials; and using the set of trans-GRIN materials toindependently control both an index of refraction distribution and anoptical dispersion distribution through a GRIN optical element.
 2. Themethod of claim 1, wherein a wavelength-dependent index of refractionfor light propagating perpendicular to the plurality of base opticalmaterials equals: a volume fraction of the first base optical materialmultiplied by a refractive index of the first base optical material,plus a volume fraction of the second base optical material multiplied bya refractive index of the second base optical material, plus one minusthe volume fraction of the first base optical material and the volume ofthe second base optical material all multiplied by the refractive indexof the third base optical material.
 3. The method of claim 1, wherein alocal refractive index at any point in the GRIN optical element is afixed function of a refractive index of each individual base opticalmaterial of the plurality of base optical materials.
 4. The method ofclaim 1, wherein the plurality of base optical materials comprisepolymer materials.
 5. The method of claim 1, wherein the plurality ofbase optical materials comprise any of polyethylene naphthalate, anisomer thereof, a polyalkylene terephthalate, a polyimide, apolyetherimide, a styrenic polymer, a polycarbonate, apoly(meth)acrylate, a cellulose derivative, a polyalkylene polymer, afluorinated polymer, a chlorinated polymer, a polysulfone, apolyethersulfone, polyacrylonitrile, a polyamide, polyvinyl acetate, apolyether-amide, a styrene-acrylonitrile copolymer, a styrene-ethylenecopolymer, poly(ethylene-1,4-cyclohexylenedimethylene terephthalate), anacrylic rubber, isoprene, isobutylene-isoprene, butadiene rubber,butadiene-styrene-vinyl pyridine, butyl rubber, polyethylene,chloroprene, epichlorohydrin rubber, ethylene-propylene,ethylene-propylene-diene, nitrile-butadiene, polyisoprene, siliconrubber, styrene-butadiene, and urethane rubber.
 6. The method of claim1, wherein the plurality of base optical materials comprise glass. 7.The method of claim 1, wherein the plurality of base optical materialscomprise different materials.
 8. A trans-gradient index (GRIN) lens,comprising: a plurality of base optical materials comprising a firstbase optical material, a second base optical material, and a third baseoptical material, wherein a wavelength-dependent index of refraction forlight propagating perpendicular to the plurality of base opticalmaterials is determined by: a volume fraction of the first base opticalmaterial combined with a refractive index of the first base opticalmaterial, a volume fraction of the second base optical material combinedwith a refractive index of the second base optical material, and oneminus the combined volume fraction of the first base optical materialand the volume of the second base optical material all multiplied by therefractive index of the third base optical material.
 9. The GRIN lens ofclaim 8, wherein the wavelength-dependent index of refraction and arefractive index dispersion through the GRIN lens are independent fromone another.
 10. The GRIN lens of claim 8, wherein a local refractiveindex at any point in the lens is a fixed function of a refractive indexof each optical material of the plurality of base optical materials. 11.The GRIN lens of claim 8, wherein the plurality of optical materialscomprise polymer materials.
 12. The GRIN lens of claim 11, wherein thepolymer materials comprise thermoplastic polymeric materials.
 13. TheGRIN lens of claim 8, wherein the plurality of base optical materialscomprise glass.
 14. The GRIN lens of claim 8, wherein the plurality ofbase optical materials comprise different materials.
 15. A systemcomprising: a fusing device that selectively combines at least threebase optical materials into one gradient index (GRIN) lens; and acontrol unit that drives the fusing device to independently control bothan index of refraction distribution and an optical dispersiondistribution through the GRIN lens.
 16. The system of claim 15, whereinthe at least three base optical materials comprise a first base opticalmaterial, a second base optical material, and a third base opticalmaterial, wherein the index of refraction distribution (n(λ)²) for lightpropagating perpendicular to the combined at least three base opticalmaterials is represented by:n(λ)²=φ_(A)n_(A)(λ)²+φ_(B)n_(B)(λ)²+(1−φ_(A)−φ_(B))n_(C)(λ)², andwherein φ_(A) is a volume fraction of the first base optical material,φ_(B) is a volume fraction of the second base optical material,n_(A)(λ)² is a refractive index of the first base optical material,n_(B)(λ)² is a refractive index of the second base optical material, andn_(C)(λ)² is a refractive index of the third base optical material. 17.The system of claim 16, wherein n_(a)(λ)<n_(b)(λ)<n_(c)(λ).
 18. Thesystem of claim 16, wherein volume fractions φ_(A) and φ_(B) are bothnon-negative values whose sum is less than
 1. 19. The system of claim15, wherein the at least three base optical materials comprise polymermaterials.
 20. The system of claim 15, wherein the at least three baseoptical materials comprise glass.